First, you were comparing the difference between
model TOA energy imbalance and observed 0 - 2000 meter OHC.
''...
the modelled TOA energy imbalance lies within error (actually, withing 1.2 SDs) of the observed value.»
Not exact matches
Figure 1: Annual average
TOA shortwave cloud forcing for present - day conditions from 16 IPCC AR4
models and iRAM (bottom center) compared with CERES satellite observations (bottom right)
b, Net
TOA flux from CERES, ERA - Interim reanalysis and the one standard deviation about the 2001 — 2010 average of 15 CMIP3
models (grey bar) are anchored to an estimate of Earth's heating rate for July 2005 — June 2010.
To touch upon Eli's so far ignored question (# 3) on bridging the hierarchy of
models: The issue at stake is the curvatuve in a plot of N vs. Ts, where N is basically the
TOA imbalance (which decays to zero as equilibrium is approached) and Ts is the surface temperature.
We have a paper (Brown et al., 2014) that showed that global
TOA energy imbalances can be internally generated and maintained for at least a decade in the CMIP5
models before the Planck Response eliminates the imbalance.
Lessons from simple toy
models and experience with more sophisticated GCMs suggests that any perturbation to the
TOA radiation budget from whatever source is a pretty good predictor of eventual surface temperature change.
There is no
modelling of any orbital variations in incoming energy, either daily, yearly or long term Milankovitch variations, based on the assumption that a global yearly average value has a net zero change over the year which is imposed on the energy forcing at the
TOA and the QFlux boundary etc..
Certainly, it is true that you can't get the stratospheric cooling in a grey
model without shortwave absorbers, not if you keep the OLR fixed (i.e. constrain things to satisfy the
TOA radiation budget).
If you can't keep up with annual - decadal changes in the
TOA radiative imbalance or ocean heat content (because of failure to correctly
model changes in the atmosphere and ocean due to natural variability), then your climate
model lacks fidelity to the real world system it is tasked to represent.
To touch upon Eli's so far ignored question (# 3) on bridging the hierarchy of
models: The issue at stake is the curvatuve in a plot of N vs. Ts, where N is basically the
TOA imbalance (which decays to zero as equilibrium is approached) and Ts is the surface temperature.
I am agreeing that convection has been
modeled, & I agree that the GCMs have included an equlibrium energy - in equals energy - out at the
TOA.
Models may be tuned to get the TOA balance right in equilibrium, but TOA balance is emergent, not enforced (and given that the models have internal variability, equilibrium is a rather fuzzy no
Models may be tuned to get the
TOA balance right in equilibrium, but
TOA balance is emergent, not enforced (and given that the
models have internal variability, equilibrium is a rather fuzzy no
models have internal variability, equilibrium is a rather fuzzy notion).
2000/2005 TSI estimates at the
TOA are 2.5 / 1.25 W / m2 or at the surface 0.43 / 0.21 W / m2 resp., it seems to me that your
model decreases solar variability, while VS inflates it.
I clearly see that the change in surface temperature and
TOA radiative forcing simulated by the
model depends upon the
model complexity, for example, how the ocean circulations are represented.
The boundary conditions in the
models are wrong —
TOA DOWN emissivity = zero.
The modelers and IPCC's use of these
models as anomalies underscores a basic problem with the ensemble, the absolute temperature values which impact
TOA.
«You're ignoring my comment above in which I clearly stated the 0.5 W / m2 was the difference between OHC and the
TOA model output.»
His 1989 Technical Report gives a lengthy description (including also the FORTRAN code) of his line - by - line HARTCODE
model, which can credibly compute the spectrally resolved outgoing
TOA radiation for a clear - sky atmosphere.
Several runs with the
model under future emissions scenarios where the radiative imbalance is known exactly and a distinct energy imbalance at
TOA was occurring nonetheless featured several stases in surface temperatures for more than a decade.
The sensitivity of an erroneous
model with an error in the albedo of 0.012 (which gives a 4 W / m ^ 2 SW
TOA flux error) to exactly the same forcing is 1.18 deg C.
«
Models fail to reproduce the observed annual cycle in all components of the albedo with any realism, although they broadly capture the correct proportions of surface and atmospheric contributions to the
TOA albedo.»
You certainly can
model with
TOA estimated average energy.
Gas laws explain our atmosphere very well, moreover, physics can not
model a greenhouse when it's hotter at
TOA.
While they are apparently called General Circulation
Models (GCM's), when it comes to CO2 effects they are apparently only about radiation at the top of the atmosphere (
TOA).
For example, Brown and Caldeira (2017) use fluctuations in Earth's top - of - the - atmosphere (
TOA) energy budget and their correlation with the response of climate
models to increases in GHG concentrations to infer that ECS lies between 3 and 4.2 K with 50 % probability, and most likely is 3.7 K. Assuming t statistics, this roughly corresponds to an ECS range that in IPCC parlance is considered likely (66 % probability) between 2.8 and 4.5 K. By contrast, Cox et al. (2018) use fluctuations of the global - mean temperature and their correlation with the response of climate
models to increases in GHG concentrations to infer that ECS likely lies between 2.2 and 3.4 K, and most likely is 2.8 K.
So it seems to me that the simple way of communicating a complex problem has led to several fallacies becoming fixed in the discussions of the real problem; (1) the Earth is a black body, (2) with no materials either surrounding the systems or in the systems, (3) in radiative energy transport equilibrium, (4) response is chaotic solely based on extremely rough appeal to temporal - based chaotic response, (5) but at the same time exhibits trends, (6) but at the same time averages of chaotic response are not chaotic, (7) the mathematical
model is a boundary value problem yet it is solved in the time domain, (8) absolutely all that matters is the incoming radiative energy at the
TOA and the outgoing radiative energy at the Earth's surface, (9) all the physical phenomena and processes that are occurring between the
TOA and the surface along with all the materials within the subsystems can be ignored, (10) including all other activities of human kind save for our contributions of CO2 to the atmosphere, (11) neglecting to mention that if these were true there would be no problem yet we continue to expend time and money working on the problem.
His
model of the atmosphere was advanced for the time, but he did consider the radiative balance at the surface, whereas we now consider that this is flawed and the balance at the top of the atmosphere (
TOA) is more appropriate.
As a consequence, like the RFTP: INST, the stratosphere - adjusted radiative forcing at the
TOA is positive over all of Antarctica and, in the
model presented herein, surface temperatures increase everywhere over that continent in response to quadrupled CO2.
The NASA
model, Prof. Johnson cites has
TOA solar radiation at 340 watts per square meter [1360 divided by 4 is 340].
How can Trenberth publish that «the
models match the
TOA energy balance» when the measurement error on the
TOA balance is ~ 5W / m ^ 2?
This popular balance
models the earth as a ball suspended in a hot fluid with heat / energy / power entering evenly over the entire
ToA spherical surface.
Well, for aerosols I took my comparison from Miller et al (2014)[iii] where it states in relation to the basic, non-interactive, NINT
model version: «Koch et al. [2011] similarly found that NINT aerosols in the year 2000 result in
TOA direct forcing of 0.40 W / m2 when using the double - call method (compared to our value of 0.00 W / m2 based upon the 1850 climate).»
The new
models assumed
TOA DOWN emissivity = 1 and black body IR from the earth's surface and the lower atmosphere.
But in a given
model you can often find ways of altering the
model's climate sensitivity through the sub-grid convection and cloud schemes that affect cloud feedback, but you have to tread carefully because the cloud simulation exerts a powerful control on the atmospheric circulation, top - of - atmosphere (
TOA) and surface radiative flux patterns, the tropical precipitation distribution, etc..
So, which
models are we talking about, and what values do they show when it comes to hindcasting and forecasting OHC,
TOA net SW radiation,
TOA net LW radiation and changing lapse rate?
The most clever
models to predict surface warming for the next century are the
models that get the
TOA radiation most correct.
Since a long - term lack of trend in GMST should indicate zero
TOA radiative flux imbalance, this implies the existence of energy leakages within those
models.
However, they will have a distorted relationship between climatological values of
TOA radiative flux variables and future warming that is not indicative of any genuine relationship between them that may exist in climate
models, let alone of any such relationship in the real climate system.
There is yet a further indicator that the approach used in the study tells one little even about the relationship in
models between the selected aspects of
TOA radiative fluxes and future warming.
Some
models are clever at hindcasting the
TOA radiation for the years 2001 to 2015.
(Other parts of the
model need to be adjusted to retrieve a good global mean
TOA energy balance but are not the main drivers of this behavior.)
This plus another basic error at
TOA creates 40 % more energy in the
models than reality, offset by exaggerated cloud cooling.
Recent
model simulations report the total anthropogenic and natural dust DRE, its components and the net effect as follows (shortwave / longwave = net
TOA, in W m — 2): H. Liao et al. (2004): — 0.21 / +0.31 = +0.1; Reddy et al. (2005a): — 0.28 / +0.14 = — 0.14; Jacobson (2001a): — 0.20 / +0.07 = — 0.13; reference case and [range] of sensitivity experiments in Myhre and Stordal (2001a, except case 6 and 7): — 0.53 -LSB--- 1.4 to +0.2] / +0.13 [+0.0 to +0.8] = — 0.4 -LSB--- 1.4 to +1.0]; and from AeroCom database
models, GISS: — 0.75 / (+0.19) = -LRB--- 0.56); UIO - CTM *: — 0.56 / (+0.19) = -LRB--- 0.37); LSCE *: — 0.6 / +0.3 = — 0.3; UMI *: — 0.54 / (+0.19) = -LRB--- 0.35).
Isaac Held here looks at how the simple two - box
models relating the globally averaged energy imbalance at the
TOA to the globally averaged surface temperature and concludes that a linear formulation deviates substantially from the behavior of GCM's.
The
TOA energy imbalance can probably be most accurately determined from climate
models and is estimated to be 0.85 ± 0.15 W m - 2 by Hansen et al. (2005) and is supported by estimated recent changes in ocean heat content (Willis et al. 2004; Hansen et al. 2005).
The sensitivity of the
models is, as I think you are saying, constrained by it's parametrizations, which are bounded by observational data on
TOA radiation data etc. (although not all very tightly constrained) but this is not what is being questioned about the
models, rather the issue is whether the
model hindcasts matching historical temperatures to some degree is evidence that they have correct physics, or is merely a result of modelers making the choices for inputs which will produce a reasonable result.
It is more plausible that the
models are running hot, that the aerosol data is botched, that the
TOA data has issues etc etc because we are trying to estimate highly spatially variable values for all global quantities with very few measurements.
In contrast to this, the calculated
TOA outgoing radiation fluxes from 11 atmospheric
models forced by the observed SST are less than the zero feedback response, consistent with the positive feedbacks that characterize these
models.
Stevens et al. has + / -0.4
TOA and + -17 «surface» which is more believable than + / -0.15 based on
models that are currently diverging from observational reality.